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Related papers: Bottomonium Spectrum with Coupled-Channel Effects

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The bottomonium spectrum up to $n = 3$ is studied within Non-Relativistic Quantum Chromodynamics up to N$^3$LO. We consider finite charm quark mass effects both in the QCD potential and the $\overline{\mathrm{MS}}$-pole mass relation up to…

High Energy Physics - Phenomenology · Physics 2018-01-29 Vicent Mateu , Pablo G. Ortega

We study the bottomonium spectrum using a relativistic potential model in the momentum space. This model is based on a complete one gluon exchange interaction with a momentum dependent screening factor to account for the effects due to…

High Energy Physics - Phenomenology · Physics 2020-07-15 David Molina , Maurizio De Sanctis , Cesar Fernández-Ramírez , Elena Santopinto

As tests of QCD in the bottomonium system, we give the most accurate results to date for the ground-state hyperfine splitting and the $\Upsilon$ leptonic width from full lattice QCD. These quantities are both accurately known from…

High Energy Physics - Lattice · Physics 2021-11-12 C. T. H. Davies , D. Hatton , J. Koponen , G. P. Lepage , A. T. Lytle

The mass spectrum of $b\bar{b}$ states has been obtained using the phenomenological relativistic quark model (RQM). The Hamiltonian used in the investigation has confinement potential and confined one gluon exchange potential (COGEP). In…

High Energy Physics - Phenomenology · Physics 2017-04-20 Manjunath Bhat , Antony Prakash Monteiro , K. B. Vijaya Kumar

The $Z_b(10610)^\pm$ and $Z_b(10650)^\pm$ are two bottomonium-like structures discovered in the $\pi h_b(mP)$, $\pi \Upsilon(nS)$ and $B^\ast\bar B^{(\ast)}+h.c.$ invariant mass spectra, where $m=\{1,2\}$ and $n=\{1,2,3\}$. Their nature is…

High Energy Physics - Phenomenology · Physics 2021-11-17 Pablo G. Ortega , Jorge Segovia , Francisco Fernandez

The mass spectrum of beauty hadrons ($b\overline{b}$ and $bbb$ baryons) and $bb$-diquarks are computed in a non-relativistic phenomenological potential model. The potential comprises of a short-range Coulomb potential, a screened…

High Energy Physics - Phenomenology · Physics 2025-08-15 Raghavendra Kaushal , Bhaghyesh

In this contribution, we discuss our recent unquenched quark model results for the spectrum of $b \bar b$ mesons with self energy corrections, due to the coupling to the meson-meson continuum. Our unquenched quark model predictions for the…

High Energy Physics - Phenomenology · Physics 2015-10-05 J. Ferretti

In this work, we adopt the one-boson exchange model to analyze the $D^{(*)}_{(s)}B^{(*)}_{(s)}$ interactions from a coupled-channel perspective. For the $I(J^{P})=1(1^{+})$ $DB^{*}/D^*B/D^*B^{*}$ system, employing the complex scaling…

High Energy Physics - Phenomenology · Physics 2025-07-23 Qing-Fu Song , Wei Liang , Qi-Fang Lü , Xiao-Nu Xiong

In this work, a comprehensive analysis of the mass spectra and decay properties of bottomonium states using a relativistic screened potential model is carried out. The mass spectrum, decay constants, $E1$ transitions, $M1$ transitions, and…

High Energy Physics - Phenomenology · Physics 2025-07-29 Chaitanya Anil Bokade , Bhaghyesh

The $\Upsilon(10753)$ state has been recently observed by the Belle and Belle~II collaborations with enough global significance to motivate an assessment of the high-energy spectrum usually predicted by any reasonable \emph{na\"ive} quark…

High Energy Physics - Phenomenology · Physics 2024-03-07 P. G. Ortega , D. R. Entem , F. Fernández , J. Segovia

In this thesis, the QCD sum rules approach has been used to study the nature of the following charmonium resonances: Y(3930), Y(4140), X(4350), Y(4260), Y(4360) and Y(4660). There is a strong evidence that these states have non-conventional…

High Energy Physics - Phenomenology · Physics 2013-06-21 Raphael M. Albuquerque

We examine the electronic width ratios of Upsilon resonances below the BBbar threshold by means of an effective (Cornell-type) QCD potential incorporating 1/m_b corrections obtained from a prior fit to the bottomonium spectrum. From our…

High Energy Physics - Phenomenology · Physics 2008-11-26 Juan-Luis Domenech-Garret , Miguel-Angel Sanchis-Lozano

We present an analysis of the mass spectrum of heavy quarkonia with non-degenerate quark masses. The heavier (bottom) valence quark is treated in a non-relativistic fashion and the other (charm) is a relativistic Wilson-like quark using the…

High Energy Physics - Lattice · Physics 2009-10-30 C. T. H. Davies , A. J. Lidsey , H. P. Shanahan

Great strides have been made in the understanding of bound states of a bottom quark $b$ and its antiquark $\bar b$ since the discovery of the first $\Upsilon$ resonances in 1977. These {\it bottomonium} bound states have a rich spectrum…

High Energy Physics - Experiment · Physics 2017-08-23 Claudia Patrignani , Todd K. Pedlar , Jonathan L. Rosner

Within the framework of dispersion theory, we analyze the dipion transitions between the lightest $\Upsilon$ states, $\Upsilon(nS) \rightarrow \Upsilon(mS) \pi\pi$ with $m < n \leq 3$. In particular, we consider the possible effects of two…

High Energy Physics - Phenomenology · Physics 2016-03-07 Yun-Hua Chen , Johanna T. Daub , Feng-Kun Guo , Bastian Kubis , Ulf-G. Meißner , Bing-Song Zou

We review the most recent experimental progress in the hadron spectroscopy, up to bottomonium mass. This covers the search for the J^PC=1^-+ exotic state, the states in J/psi decays, the spin-singlets of heavy quarkonium, and the…

High Energy Physics - Experiment · Physics 2011-08-04 Chang-Zheng Yuan

The bottom-charmed ($B_c$) mesons are more stable than their charmonium ($c\bar c$) and bottomium ($b\bar b$) partners because they cannot annihilate into gluons. However, the low production cross-sections and signal-to-background ratios…

High Energy Physics - Phenomenology · Physics 2020-04-22 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernandez

Many charmonium-like and bottomonium-like $XYZ$ resonances have been observed by the Belle, Babar, CLEO and BESIII collaborations in the past decade. They are difficult to fit in the conventional quark model and thus are considered as…

High Energy Physics - Phenomenology · Physics 2014-11-04 Wei Chen , J. Ho , T. G. Steele , R. T. Kleiv , B. Bulthuis , D. Harnett , T. Richards , Shi-Lin Zhu

Compared to charmonium-like states, exotic hadrons associated with $b$-quark offer distinct advantages for exploring the nature of multiquark phenomena and the dynamics of the strong interaction. Due to the heavier bottom quark mass,…

High Energy Physics - Phenomenology · Physics 2026-03-11 Xinchen Dai , Sen Jia , Alexey Nefediev , Juan Nieves , Chengping Shen , Liming Zhang

We study the energy spectrum of bottomonium in perturbative QCD, taking alpha_s(Mz)=0.1181 +/- 0.0020 as input and fixing m_b^{MSbar}(m_b^{MSbar}) on the Upsilon(1S) mass. Contrary to wide beliefs, perturbative QCD reproduces reasonably…

High Energy Physics - Phenomenology · Physics 2009-06-12 N. Brambilla , Y. Sumino , A. Vairo